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Future directions: magnon probes and spin flips

3. Spin control in antiferromagnets using magnetic THz transients 10

3.5. Future directions: magnon probes and spin flips

We have successfully demonstrated the coherent control of ultrafast spin precession in antiferromagnetic NiO using the Zeeman torque of an intense THz transient. Such a control scheme is minimally invasive (as it leaves the non-spin degrees of freedom of the NiO in their ground state) and universal (as it is mediated by the Zeeman interaction). Coherent magnons may now be used as probes for ultrafast interactions of electron spin with orbital motion and lattice modes in essentially all THz-transparent matter and at all relevant frequencies.

We emphasize that Zeeman-driven spin motion is expected to be widely scalable, and our simulations based on equation (7) indicate a novel regime of dramatic THz nonlinearities beyond the perturbative regime. In contrast to the weak-field regime (figure7(a)), THz peak amplitudes of 11 T lead to oscillations ofS1x significantly slower than the high-frequency magnon at 1 THz, and the evolution of S1y is dominated by the low-frequency magnon at≈0.2 THz (figure7(b)).

Note that both signals exhibit a modulation depth of nearly 100 %. Most remarkably, the change of S1z from 1 to nearly −1 demonstrates the induction of a spin flip, which also becomes apparent in an image of the three-dimensional spin trajectory (figure7(d)). It is not obvious whether in such an extreme excitation regime the parameters of the spin Hamiltonian of equation (6) can still be assumed to be constant. However, recent modeling based on an extended Hamiltonian has demonstrated similar magnetization dynamics [52]. In any case, future studies of high-field-driven THz spin dynamics will enter an entirely new territory of many-body physics.

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Figure 7. Simulated dynamics of sublattice spin S1 (a) under the excitation conditions used in the experiment (peak driving field 0.14 T) and (b) with a peak field of 11 T. (c, d) Three-dimensional spin trajectories resulting from (a) and (b), respectively. In (c), spin deflections are numerically enhanced for better visibility.

4. Conclusions and perspectives

Intense electric and magnetic multi-THz fields have become versatile tools to selectively and coherently control electronic or spin degrees of freedom of condensed matter in a previously elusive spectral range, and in the sub-optical-cycle temporal regime. Our study of multi-THz two-dimensional spectroscopy confirms the onset of a non-perturbative response under even off-resonant excitation of interband transitions in InSb. Peak electric fields above 5 MV cm−1 lead to carrier-wave Rabi flopping between the valence and conduction bands. These results underpin the large potential of novel strong-field multi-THz technology for high harmonics generation [53] and coherent quantum control of low-energy excitations [22, 54]. The unique capability of field-sensitive multi-dimensional spectroscopy to separate purely coherent and incoherent nonlinearities may open a new chapter in the investigation of collective low-energy excitations including inter-molecular vibrations in hydrogen-bonded liquids [55] and Cooper pair breaking transitions in superconductors [56]. On the other hand, all-magnetic spin control opens the door to the new concept of THz electron spin resonance. Coherent magnons in systems as diverse as ferro- and antiferromagnets or high-temperature superconductors may, for instance, be employed as unique probes of ultrafast interactions with lattice and charge degrees of freedom. Furthermore, our experiments may inspire the development of ultrafast next-generation memory devices, spin-based quantum computation and spintronics. This is only the beginning of a new era of sub-cycle multi-THz coherent control of condensed matter.

Acknowledgments

We thank A Leitenstorfer, M Wolf, M Fiebig, B Mayer, O Schubert, F Junginger, S M¨ahrlein, C Schmidt, G Klatt and T Dekorsy for ongoing collaborations which laid the basis for this work. We also appreciate fruitful discussions with T Cocker, D Seletskiy, M P Hasselbeck and M Sheik-Bahae. Financial support by Deutsche Forschungsgemeinschaft (DFG) through projects PA 2113/1-1 and HU 1598/1-1 as well as by the European Research Council via ERC Starting Grant QUANTUMsubCYCLE is gratefully acknowledged.

References

[1] Tonouchi M 2007 Cutting-edge terahertz technologyNature Photon.197–105

[2] Ulbricht R, Hendry E, Shan J, Heinz T F and Bonn M 2011 Carrier dynamics in semiconductors studied with time-resolved terahertz spectroscopyRev. Mod. Phys.83543–86

[3] Sell A, Scheu R, Leitenstorfer A and Huber R 2008 Field-resolved detection of phase-locked infrared transients from a compact Er:fiber system tunable between 55 and 107 THzAppl. Phys. Lett.93251107 [4] Ashida M 2008 Ultra-broadband terahertz wave detection using photoconductive antennaJapan J. Appl. Phys.

478221–5

[5] G¨unter G, Anappara A A, Hees J, Sell A, Biasiol G, Sorba L, De Liberato S, Ciuti C, Tredicucci A, Leitenstorfer A and Huber R 2009 Sub-cycle switch-on of ultrastrong light–matter interaction Nature 458178–81

[6] Bartel T, Gaal P, Reimann K, Woerner M and Elsaesser T 2005 Generation of single-cycle THz transients with high electric-field amplitudesOpt. Lett.302805–7

[7] Blanchard Fet al 2011 Generation of intense terahertz radiation via optical methodsIEEE J. Sel. Topics Quantum Electron.175–16

[8] Hebling J, Yeh K-L, Hoffmann M C, Bartal B and Nelson K A 2008 Generation of high-power terahertz pulses by tilted-pulse-front excitation and their application possibilitiesJ. Opt. Soc. Am.B25B6–19 [9] Hirori H, Doi A, Blanchard F and Tanaka K 2011 Single-cycle terahertz pulses with amplitudes exceeding

1 MV cm1generated by optical rectification in LiNbO3Appl. Phys. Lett.98091106

[10] Minami Y, Kurihara T, Yamaguchi K, Nakajima M and Suemoto T 2013 High-power THz wave generation in plasma induced by polarization adjusted two-color laser pulsesAppl. Phys. Lett.102041105

[11] Razzari Let al2009 Nonlinear ultrafast modulation of the optical absorption of intense few-cycle terahertz pulses inn-doped semiconductorsPhys. Rev.B79193204

[12] Su F Het al2009 Terahertz pulse induced intervalley scattering in photoexcited GaAsOpt. Express179620–9 [13] Turchinovich D, Hvam J M and Hoffmann M C 2012 Self-phase modulation of a single-cycle terahertz pulse

by nonlinear free-carrier response in a semiconductorPhys. Rev.B85201304

[14] Kuehn W, Gaal P, Reimann K, Woerner M, Elsaesser T and Hey R 2010 Terahertz-induced interband tunneling of electrons in GaAsPhys. Rev.B82075204

[15] Hoffmann M C, Hebling J, Hwang H Y, Yeh K-L and Nelson K A 2009 Impact ionization in InSb probed by terahertz pump—terahertz probe spectroscopyPhys. Rev.B79161201

[16] Hirori H, Shinokita K, Shirai M, Tani S, Kadoya Y and Tanaka K 2011 Extraordinary carrier multiplication gated by a picosecond electric field pulseNature Commun.2594

[17] Blanchard F et al2011 Effective mass anisotropy of hot electrons in nonparabolic conduction bands of n-doped InGaAs films using ultrafast terahertz pump–probe techniquesPhys. Rev. Lett.107107401 [18] Katayama I, Aoki H, Takeda J, Shimosato H, Ashida M, Kinjo R, Kawayama I, Tonouchi M, Nagai M and

Tanaka K 2012 Ferroelectric soft mode in a SrTiO3thin film impulsively driven to the anharmonic regime using intense picosecond terahertz pulsesPhys. Rev. Lett.108097401

[19] Rini M, Tobey R, Dean N, Itatani J, Tomioka Y, Tokura Y, Schoenlein R W and Cavalleri A 2007 Control of the electronic phase of a manganite by mode-selective vibrational excitationNature44972–4

[20] Dienst A, Hoffmann M C, Fausti D, Petersen J C, Pyon S, Takayama T, Takagi H and Cavalleri A 2011 Bi-directional ultrafast electric-field gating of interlayer charge transport in a cuprate superconductorNature Photon.5485–8

[21] Luo C W, Reimann K, Woerner M, Elsaesser T, Hey R and Ploog K H 2004 Phase-resolved nonlinear response of a two-dimensional electron gas under femtosecond intersubband excitationPhys. Rev. Lett.92047402 [22] Leinß S, Kampfrath T, Volkmann K v., Wolf M, Steiner J T, Kira M, Koch S W, Leitenstorfer A and Huber R

2008 Terahertz coherent control of optically dark paraexcitons in Cu2OPhys. Rev. Lett.101246401 [23] Kuehn W, Gaal P, Reimann K, Woerner M, Elsaesser T and Hey R 2010 Coherent ballistic motion of electrons

in a periodic potentialPhys. Rev. Lett.104146602

17

[24] Zaks B, Liu R B and Sherwin M S 2012 Experimental observation of electron-hole recollisions Nature 483580–3

[25] Fleischer S, Zhou Y, Field R W and Nelson K A 2011 Molecular orientation and alignment by intense single-cycle THz pulsesPhys. Rev. Lett.107163603

[26] Fleischer S, Field R W and Nelson K A 2012 Commensurate two-quantum coherences induced by time-delayed THz fieldsPhys. Rev. Lett.109123603

[27] Sell A, Leitenstorfer A and Huber R 2008 Phase-locked generation and field-resolved detection of widely tunable terahertz pulses with amplitudes exceeding 100 MV cm1Opt. Lett.332767–9

[28] Junginger F, Sell A, Schubert O, Mayer B, Brida D, Marangoni M, Cerullo G, Leitenstorfer A and Huber R 2010 Single-cycle multiterahertz transients with peak fields above 10 MV cm1Opt. Lett.352645–7 [29] Wegener M 2004Extreme Nonlinear Optics1st edn (Berlin: Springer)

[30] Yamaguchi K, Nakajima M and Suemoto T 2010 Coherent control of spin precession motion with impulsive magnetic fields of half-cycle terahertz radiationPhys. Rev. Lett.105237201

[31] Zhou R, Jin Z, Li G, Ma G, Cheng Z and Wang X 2012 Terahertz magnetic field induced coherent spin precession in YFeO3Appl. Phys. Lett.100061102

[32] Junginger F, Mayer B, Schmidt C, Schubert O, M¨ahrlein S, Leitenstorfer A, Huber R and Pashkin A 2012 Nonperturbative interband response of a bulk InSb semiconductor driven off resonantly by terahertz electromagnetic few-cycle pulsesPhys. Rev. Lett.109147403

[33] Kampfrath T, Sell A, Klatt G, Pashkin A, Ma S, Dekorsy T, Wolf M, Fiebig M, Leitenstorfer A and Huber R 2011 Coherent terahertz control of antiferromagnetic spin wavesNature Photon.531–4

[34] Hebling J, Hoffmann H C, Hwang H Y, Yeh K-L and Nelson K A 2010 Observation of nonequilibrium carrier distribution in Ge, Si and GaAs by terahertz pump— terahertz probe measurementsPhys. Rev.B81035201 [35] Kuehn W, Reimann K, Woerner M and Elsaesser T 2009 Phase-resolved two-dimensional spectroscopy based

on collinear n-wave mixing in the ultrafast time domainJ. Chem. Phys.130164503

[36] Olszak P D, Cirloganu C M, Webster S, Padilha L A, Guha S, Gonzalez L P, Krishnamurthy S, Hagan D J and van Stryland E W 2010 Spectral and temperature dependence of two-photon and free-carrier absorption in InSbPhys. Rev.B82235207

[37] Sheik-Bahae M, Rossi T and Kwok H S 1987 Frequency dependence of the two-photon absorption coefficient in InSb: tunneling effectsJ. Opt. Soc. Am.B41964–9

[38] Yuen S Y and Wolff P A 1982 Difference-frequency variation of the free-carrier-induced, third-order nonlinear susceptibility in n-InSbAppl. Phys. Lett.40457–9

[39] Hutchings D C, Sheik-Bahae M, Hagan D J and van Stryland E W 1992 Kramers-Kronig relations in nonlinear opticsOpt. Quantum Electron.241–30

[40] Ziolkowski R W, Arnold J M and Gogny D M 1995 Ultrafast pulse interactions with two-level atomsPhys.

Rev.A523082–94

[41] Thomas Andrews J and Sen P 1998 Effect of non-centrosymmetry on stark broadening in bulk indium antimonide crystalQuantum Semiclass. Opt.10663

[42] M¨ucke O D, Tritschler T, Wegener M, Morgner U and K¨artner F X 2001 Signatures of carrier-wave rabi flopping in GaAsPhys. Rev. Lett.87057401

[43] Tritschler T, M¨ucke O D and Wegener M 2003 Extreme nonlinear optics of two-level systemsPhys. Rev.A 68033404

[44] Ghimire S, DiChiara A D, Sistrunk E, Agostini P, DiMauro L F and Reis D A 2011 Observation of high-order harmonic generation in a bulk crystalNature Phys.7138–41

[45] Merlin R 2009 Metamaterials and the Landau-Lifshitz permeability argument: large permittivity begets high-frequency magnetismProc. Natl Acad. Sci. U.S.A.1061693–8

[46] Hiebert W K, Stankiewicz A and Freeman M R 1997 Direct observation of magnetic relaxation in a small permalloy disk by time-resolved scanning kerr microscopyPhys. Rev. Lett.791134–7

[47] Back C H, Allenspach R, Weber W, Parkin S S P, Weller D, Garwin E L and Siegmann H C 1999 Minimum field strength in precessional magnetization reversalScience285864–7

[48] Wang Z, Pietz M, Walowski J, F¨orster A, Lepsa M I and M¨unzenberg M 2008 Spin dynamics triggered by subterahertz magnetic field pulsesJ. Appl. Phys.103123905

[49] Kirilyuk A, Kimel A V and Rasing T 2010 Ultrafast optical manipulation of magnetic orderRev. Mod. Phys.

822731–84

[50] S¨anger I, Pavlov V V, Bayer M and Fiebig M 2006 Distribution of antiferromagnetic spin and twin domains in NiOPhys. Rev.B74144401

[51] Hutchings M T and Samuelsen E J 1972 Measurement of spin-wave dispersion in NiO by inelastic neutron scattering and its relation to magnetic propertiesPhys. Rev.B63447–61

[52] Wienholdt S, Hinzke D and Nowak U 2012 THz switching of antiferromagnets and ferrimagnetsPhys. Rev.

Lett.108247207

[53] Golde D, Meier T and Koch S W 2008 High harmonics generated in semiconductor nanostructures by the coupled dynamics of optical inter- and intraband excitationsPhys. Rev.B77075330

[54] Cole B E, Williams J B, King B T, Sherwin M S and Stanley C R 2001 Coherent manipulation of semiconductor quantum bits with terahertz radiationNature41060–3

[55] Cowan M L, Bruner B D, Huse N, Dwyer J R, Chugh B, Nibbering E T J, Elsaesser T and Miller R J D 2005 Ultrafast memory loss and energy redistribution in the hydrogen bond network of liquid H2ONature 434199–202

[56] Papenkort T, Kuhn T and Axt V M 2008 Coherent control of the gap dynamics of BCS superconductors in the nonadiabatic regimePhys. Rev.B78132505